# Patent

## Title
Magnetic proximity sensor system and associated methods of sensing a magnetic field

## Abstract

A magnetic proximity sensor is attached to a ferrous object such that the sensor alerts a practitioner if a threshold of magnetic strength has been exceeded by bringing the ferrous object within a certain proximity to the magnet of an MRI scanner. The magnetic proximity sensor includes at least one magnetic field sensor for sensing a magnetic field strength. An alarm in communication with the field sensor alerts a practitioner that a threshold of magnetic strength has been exceeded. A battery powers the field sensor and the alarm. The field sensor may produce an output voltage corresponding to the sensed magnetic field strength, and a potentiometer may provide a reference voltage corresponding to a threshold magnetic field strength. A comparator compares the reference voltage to the output voltage, and triggers an alarm if the output voltage exceeds the reference voltage.

## Background
RELATED APPLICATIONS
This application claims priority of U.S. Provisional Application No. 61/041,886, filed Apr. 2, 2008, incorporated herein by reference.


BACKGROUND
Since its introduction, magnetic resonance imaging (MRI) has provided physicians and clinicians with an unparalleled window into the human body. Using a magnetic field in combination with radio waves, MRI produces detailed images of internal organs and body systems, without subjecting a patient to the radiation incurred during traditional x-ray or CT scan procedures. A strong magnet contained in an MRI scanner generates a field which causes molecules in the body to align. The molecules are briefly excited by radio waves as they return to their original condition. During this process, the molecules emit signals that are received and converted into images by a computer. The procedure itself is painless and, in some cases, may eliminate hospitalization for other diagnostic testing and costs associated therewith. The MRI procedure itself is quite safe—the imaging does not damage body tissues.
Despite the apparent advantages of MRI, the potential for interaction between the MRI scanner and ferrous metal objects, either internal or external to the patient, is cause for concern. For example, the MRI magnet (typically 5,000 to 20,000 Gauss, although magnets as strong as 30,000 Gauss are now available) may move internal objects such as metal pins or plates within a patient's body, and may interfere with the functioning of a pacemaker. External metallic objects ranging from hairpins to crash carts have been projectilized by the magnetic field of MRI scanners, causing injury, and even death, to patients undergoing the procedure and to attending staff. In one well-publicized 2001 accident, a six year-old boy undergoing MRI was killed when an oxygen tank was pulled into the bore of the scanner. When brought within reach of the magnetic field, the oxygen tank flew into the scanner and fractured the boy's skull, causing a fatal cerebral hemorrhage.
SUMMARY
In one embodiment, a magnetic proximity sensor system includes a magnetic field sensor for sensing a magnetic field strength. An alarm in communication with the field sensor alerts a practitioner if a threshold of magnetic strength has been exceeded.
In one embodiment, a magnetic proximity sensor system includes a magnetic field sensor for sensing an external magnetic field and generating an output voltage corresponding to a strength of the magnetic field. A potentiometer produces a reference voltage corresponding to a threshold magnetic field strength, and a comparator compares the reference voltage to the output voltage. An alarm in communication with the comparator indicates when the output voltage exceeds the reference voltage.
In one embodiment, a magnetic proximity sensor system has a plurality of field sensors for sensing a positive or a negative external magnetic field and for generating output voltages corresponding to a strength of the positive or negative magnetic field. A first potentiometer produces a first reference voltage corresponding to a threshold of positive magnetic field strength. A first comparators in communication with the first potentiometer and the field sensors, compares the first reference voltage to the output voltages, to determine whether the output voltages exceed the first reference voltage. A second potentiometer produces a second reference voltage corresponding to a threshold of negative magnetic field strength. A second comparator, in communication with the second potentiometer and the field sensors, compares the second reference voltage to the output voltages, to determine whether the output voltages exceed the first reference voltage. An alarm in communication with the first and second comparators indicates when the output voltages exceed the first or the second reference voltage.
In one embodiment, a method of detecting magnetic field strength includes sensing a magnetic field with at least one magnetic field sensor, and generating an output voltage corresponding to a strength of the magnetic field. A reference voltage is provided and compared to the output voltage. If the output voltage is greater than the reference voltage, an alarm is activated.
In one embodiment, a method for preventing magnetic interaction between a mobile ferrous object and an MRI scanner includes attaching a magnetic proximity sensor to the ferrous object and sensing an external magnetic field with the magnetic proximity sensor. An alarm is generated if the sensed external magnetic field exceeds a threshold magnetic field strength.



BRIEF DESCRIPTION OF DRAWINGS
FIG. 1 is a schematic illustration of a magnetic proximity sensor system.
FIG. 2 is a schematic illustration of a magnetic proximity sensor system with a Hall Effect sensor.
FIG. 3A is a top view of a magnetic proximity sensor system as detailed in FIG. 1 or FIG. 2.
FIG. 3B is a back view of the magnetic proximity sensor system of FIG. 3A with an adhesive backing.
FIG. 3C is a back view of the magnetic proximity sensor system of FIG. 3A, with a fastener.
FIG. 4 is a schematic illustration of a magnetic proximity sensor system with internal Hall effect sensors, comparators and potentiometers.
FIG. 5 is a schematic illustration of a magnetic proximity sensor system with internal reed switches.
FIG. 6A is a side view of one modified reed switch, for use with the magnetic proximity sensor system of FIG. 5.
FIG. 6B is a side view of the modified reed switch of FIG. 6A, in closed-circuit position.
FIG. 7A is a side view of another modified reed switch, for use with the magnetic proximity sensor system of FIG. 5.
FIG. 7B is a side view of the modified reed switch of FIG. 7A, in closed-circuit position.
FIG. 8 is a flowchart illustrating one method of detecting a magnetic field using a magnetic proximity sensor system of FIGS. 1-4.
FIG. 9 is a flowchart illustrating one method of detecting a threshold magnetic field strength using a magnetic proximity sensor with the modified reed switches of FIGS. 6A-6B and/or 7A-7B.



DETAILED DESCRIPTION
The disclosed magnetic proximity sensor system is designed to alert a practitioner (e.g., a physician, technologist, anesthesiologist or attending MRI staff) that a movable metal object (e.g., a crash cart, oxygen tank or metallic bucket) has passed beyond a threshold of magnetic strength (e.g., 20 Gauss). The allowable magnetic strength can be preset, thereby allowing appropriate intervention before the metal object gets too close to the MRI scanner magnet.
The magnetic proximity sensor system is intended to add a layer of safety for practitioners and patients so that appropriate boundaries are respected for hardware that has magnetic properties but that still needs to be in the scanner room. FIG. 1 shows one embodiment of a magnetic proximity sensor system 100. System 100 includes a magnetic field sensor 102, an alarm 104 and a battery 106. Field sensor 102 is for example a magnetic reed switch or a Hall effect semiconductor switch. A Hall effect semiconductor switch may enhance directional sensitivity of the sensor as compared to a conventional reed switch; however, a modified reed switch (described herein with respect to FIGS. 5, 6 and 7) may provide directional sensitivity comparable to the Hall effect switch, while improving power efficiency of system 100.
Alarm 104 may be a buzzer, bell, beeper or similar noise making device that outputs an audible signal. A speaker 108 broadcasts the signal from alarm 104, and an optional amplifier 110 amplifies the signal. Alarm 104 may alternatively be, or optionally include, a visual alarm, such as a flashing or blinking light, to provide awareness of the magnetic proximity sensor in loud environments, such as an MRI suite. Field sensor 102 may also include a tactile alarm, for example vibrating upon play of the alarm signal, to further draw attention. Battery 106 can be alkaline or lithium and for example ranges from 3-6 Volts. Alarm 104 is for example triggered when field sensor 102 detects a five Gauss magnetic field level. This level corresponds to the generally recognized “safe distance” from an MRI scanner.
FIG. 2 shows an embodiment of a magnetic proximity sensor system 200 with a Hall effect sensor 202. Hall effect sensor 202 uses a potentiometer 203 to create a voltage, used to set an alarm 204 to the desired Gauss default (e.g., five). Potentiometer 203 can be a commercially available potentiometer such as the 10k Bourns 3262 Trimming Potentiometer or a Spectral 50k 43P503. The power source for proximity sensor system 200 is important because calibration of the Hall effect sensor 202 relies on the voltage through the circuit. Battery 206 is, for example, a 6 Volt 23-469 Radio Shack Alkaline. Alarm 204 is a sound device (e.g., a bell or buzzer) with an average decibel output that is louder than the ambient noise in an MRI facility. Alarm 204 for example emits sound rated at about 90 dB. This approximately 30 dB louder than the ambient noise of an average MRI facility. Although medical personnel and objects generally do not enter the MRI room during imaging, alarm 204 may also be louder than the ambient noise in an MRI room during imaging; this guards against metal objects being brought too close to a functioning MRI scanner if medical personnel must enter the MRI room during scanning, due to an emergency. To draw attention in a loud environment (e.g., during scanning), alarm 204 may include (or may alternatively be) the visual and tactile features described above with respect to FIG. 1.
Comparator 208 compares the voltage from the Hall effect sensor 202 to potentiometer 203. A commercially available comparator is acceptable such as the LM339 low power low offset voltage quad comparator. When voltage from the Hall Sensor is higher than voltage from potentiometer 203, then the magnetic field acting on the device has exceeded the level setting, e.g., five Gauss.
FIG. 3A shows a top view of a magnetic proximity sensor system 300. Magnetic proximity sensor system 300 for example includes the components discussed with respect to FIG. 1 or FIG. 2. Sensor system 300 includes a body 301. As shown in FIG. 3A, body 301 is circular or coin-shaped; however, body 301 may be formed as a square, rectangle, star or other geometric or abstract shape.
Body 301 includes an outer casing 302 enclosing a potting material 303. Outer casing 302 encases the entire circuit (see FIG. 1, 2) except an emitting portion (e.g., a speaker) of an alarm (e.g., a visual, tactile and/or audible alarm) 304. Potting material 303 may be plastic, silicon or any substantially hard and durable material, such as potting resin CR 300, for coating and protecting internal components of sensor system 300. Casing 302 may be an outer surface of potting material 303, for example when sensor system 300 is formed by hardening a portion of potting material 303 around internal components (e.g., by pouring potting material 303 into a mold). Positive and negative connectors 306 and 308 optionally extend from potting material 303 and casing 302 in order to connect to an external battery. Alternately, electrical connections/contacts (e.g., a plug or a cord) for connecting to an external power source may be provided with casing 302.
FIG. 3B is a back view of the magnetic proximity sensor system 300. In one embodiment, an optional adhesive device 310 is used to secure system 300 to a mobile ferrous object. Adhesive device 310 may be a tape, glue or other suitable adhesive. Optionally, as shown in FIG. 3C, a fastener 312 is provided with magnetic proximity sensor system 300. Fastener 312 is shown as a clip attached to a back surface of system 300; however, fastener 312 may be any fastener suitable for attaching system 300 to the mobile ferrous object, such as a clamp, strap, snap or Velcro. Likewise, fastener 312 may be provided elsewhere on system 300, e.g., on a top, bottom or side surface.
FIG. 4 schematically shows a magnetic proximity sensor system 400. System 400 includes three Hall effect sensors 402, for sensing magnetic fields along x, y and z planes, indicated by coordinates 403. Hall effect sensors 402 are for example bipolar Hall sensors such as the Melexis' Linear Hall Effect Sensor MLX90215 LCO3. Two potentiometers 404A and 404B create an electrical current through Hall effect sensors 402. Potentiometer 404A is for example set to provide a voltage sufficient to trigger an alarm 406 when sensors 402 detect a magnetic field greater than positive five Gauss. Potentiometer 404B is for example set to provide a voltage sufficient to trigger alarm 406 when sensors 402 detect magnetic field stronger than negative five Gauss. Comparators 408A and 408B compare the fixed voltages provided by potentiometers 404A and 404B, respectively, with voltages from Hall effect sensors 402. For example, when comparator 408A determines that the voltage from Hall sensors 402 is greater than the voltage provided by potentiometer 404A, then the magnetic field acting upon sensor system 400 has exceeded five Gauss.
Upon detecting a magnetic field beyond the default threshold (e.g. five Gauss), alarm 406 is triggered. An optional speaker 410 may be provided to broadcast output from alarm 406, or alarm 406 may include a sound emitting portion. For example, alarm 406 may be a miniature buzzer such as the Radio Shack 12VDC Piezo Mini Buzzer 273-074. Comparators 408A and 408B may be small, multi-comparator chips such as LM 339 quad-comparator chips by National Semiconductor. Potentiometers 404A, 404B are for example variable resistors such as the 10K Bourns 3262. A battery 412 powers sensors 402, potentiometers 404, alarm 406 and comparators 408. Battery 412 may also provide power to one or more capacitors (not shown). For example, 10 μF capacitor and a 0.1 μF capacitor may be included with sensor system 400, to minimize voltage variances in internal circuitry.
Battery 412 may be contained within a housing 414, along with the above-mentioned components and circuitry of magnetic proximity sensor system 400. Optionally, electrical connections/contacts may be provided with sensor system 400 such that sensor system 400 is connectable to an external battery or power source. Alarm 406 or speaker 410 may be surrounded but not covered by housing 414, to allow for sound emission.
Housing 414 may surround or be formed by a potting material 416. Potting material 416 is for example a plastic, silicon or other durable material such as potting resin CR 300. Sensor system 400 may be formed by placing potting material 416 and sensors 402, potentiometers 404, alarm 406, comparators 408, speaker 410 and battery 412 in a mold. Once hardened, an outer layer of potting material 416 forms housing 414. An on/off switch or button 418 may be provided to conserve battery power when sensor system 400 is not in use.
FIG. 5 schematically shows a magnetic proximity sensor system 420, with two modified reed switches 422 for multidirectional sensing of magnetic fields. System 420 includes a housing 424. Housing 424 may be formed from a potting material 426, as described above with respect to sensor system 400, FIG. 4. Potting material 426 is for example a plastic, silicon or other durable material such as potting resin CR 300. Although reed switches 422 do not require power to operate, an on/off switch or button (e.g., button 418) may be provided to conserve battery power (e.g., drain by an included alarm) when system 420 is not in use. In one embodiment, due to the low power requirements of system 420 and to assuage safety concerns, system 420 does not include an on off switch or button, but is constantly powered by the battery. An additional low battery indicator (not shown) such as a light, may also connect with the battery and be visible on or through housing 424. Optionally, external contacts are provided through housing 424 (e.g., as described with respect to FIG. 3A) for connection with an external power source. An “on” indicator, e.g., a green light, may be provided with housing 424, to indicate that the system is properly connected.
Modified reed switches 422 are placed perpendicular to one another, for sensing magnetic fields along x, y and z axes, illustrated by coordinates 403. Each modified switch 422 may be tripped in two axes, thus, two perpendicular switches 422 provide for sensing of magnetic fields along x, y and z axes. A third modified reed switch 422, or a standard reed switch, may be added to sensor system 420 to enhance multi-directional sensitivity.
Modified reed switches 422 are connected to alarm 428, which is powered for example by battery 412. Alarm 428 is triggered upon breach of a magnetic field threshold and completion of a switch 422 circuit. Magnetic field threshold may be engineered into modified switches 422, as described below with respect to FIGS. 6 and 7. Housing 424 may be formed around an outlet or speaker of Alarm 428, or alarm 428 may be broadcast through a separate speaker configured with housing 424 (e.g., speaker 412, FIG. 4). Resistors 430 may be included with switches 422 or as separate components of system 420 that provide connection with alarm 428, where limitation of current through system 420 is desired.
FIGS. 6A and 6B are schematic views of one modified reed switch 422. Modified switch 422 includes a circular or hemispheric conductive contact 432 and a magnetic contact 434. An end 436 of magnetic contact 434 is centered within hemispheric contact 432. Magnetic contact 434 may be anchored at its other end by a housing 438 of modified reed switch 422. Housing 438 is for example made of glass. In one embodiment, magnetic contact 434 includes a wire filament 440 within a nonconductive sheath 442, with a ferrous end 436 extending from the sheath. Sheath 442 is for example a stiffening monofilament or polymer that supports the weight of magnetic contact 434, yet flexes to allow contact between ferrpus end 436 and hemispheric contact 432 (and completion of the switch circuit) at an appropriate magnetic field strength or threshold. The magnetic threshold of each switch 422 may be customized by varying strength and/or stiffness of sheath 442, for example by varying sheath 442 composition.
Hemispheric contact 432 is conductive but not magnetic, and is stabilized within housing 438 by one or more supports 444. In one embodiment, hemispheric contact 432 is a copper ring with four extending copper tabs 444 and a connected wire 446. Magnetic contact 434 is supported by a nonconductive polymer sheath 442 with sufficient stiffness to hold wire filament 440 (and ferrous end 436) away from hemispheric contact 432, as shown in FIG. 6A, until an external magnetic field exceeds five Gauss. Once the five gauss threshold is exceeded, magnetic contact 434 is deflected by the external magnetic field, for example in the direction of arrow 448, into contact with hemispheric contact 432, as shown in FIG. 6B, closing the switch circuit. It will be appreciated that reed switch 444 may be deflected, or triggered, along two axes and not solely in the direction of arrow 448.
Reed switch 444 is connected with (e.g., wired to) battery powered alarm 438, optionally via a resistor 430 (see FIG. 4). Completion of the switch circuit (FIG. 6B) triggers alarm 438, which sounds, flashes and/or vibrates to indicate that the threshold magnetic field has been breached. When external magnetic field strength decreases (for example as a practitioner moves a crash cart with an attached sensor 420 away from an MRI machine), force exerted by sheath 442 overcomes the decreasing magnetic field and returns magnetic contact 434 to the open position of FIG. 6A. The stationary nature of hemispheric contact 432 may prevent or reduce contact magnetization, as has been observed with traditional reed switches.
FIGS. 7A and 7B are schematic views showing an alternate modified reed switch 450 in open and closed positions, respectively. Modified switch 450 has a housing 452 encasing a magnetic contact 454. In one embodiment, magnetic contact 454 is a ferromagnetic contact with a ferrous contact end or bead 456 on a wire 458. Housing 452 is for example made of glass. Ferromagnetic contact 454 is supported by a stiffening monofilament or monofilaments 460 that connect with bead 456 and extend the length l of modified switch 450. Ferromagnetic contact 454 is positioned such that ferrous bead 456 is centered at a diameter of hemispheric contact 462 when switch 450 is open (FIG. 7A). Hemispheric contact 462 is a conductive, non-magnetic material, such as copper, with a connected wire 464. As with hemispheric contact 432 of FIGS. 6A and 6B, hemispheric contact 462 may include one or more supports (not shown) to secure it within housing 452. Alternately, housing 452 may be formed with a recess and/or extrusions to hold hemispheric contact 462 in place.
Modified switch 450 has a magnetic threshold that is for example governed by the strength or stiffness of monofilament(s) 460. When switch 450 is in the presence of a magnetic field powerful enough to overcome the stiffening properties of monofilament(s) 460, ferromagnetic contact 454 bends, flexing monofilament(s) 460, to contact hemispheric contact 462 and close the switch circuit, as shown in FIG. 7B. It will be appreciated that as with switch 422, switch 450 may be triggered, or ferromagnetic contact 454 bent, along two axes. When the magnetic field affecting switch 450 decreases, for example as a sensing system incorporating switch 450 is moved away from an MRI machine or other magnetic source, the stiffening properties of monofilament(s) 460 aid in returning ferromagnetic contact 454 to its original, or open position (see FIG. 7A).
Exemplary use of the above-described magnetic proximity sensor systems 100-400 is illustrated in the flow chart of FIG. 8. Exemplary use of a magnetic proximity sensor with modified reed switches, e.g., system 420, is illustrated in the flow chart of FIG. 9.
In particular, FIG. 8 depicts a method 500 for detecting a magnetic field using one of such magnetic proximity sensor systems. The magnetic proximity sensor system is attached to a metal (e.g., ferrous) object, in step 502. If an on/off switch, power button or other input is provided, the magnetic proximity sensor system is turned on (e.g., via switch 418, FIG. 4), in step 504. In an example of steps 502, 504, system 400 is attached to a mobile ferrous object such as a clipboard, crash cart or oxygen tank, and turned on.
A fixed voltage corresponding to a threshold magnetic field strength is provided, in step 506. An external magnetic field is sensed, in step 508, and translated into an output voltage, in step 510. The output voltage is compared with the fixed voltage, in step 512. In an example of steps 506-512, potentiometer 404 provides a fixed voltage. Potentiometer 404 is for example set to generate a fixed voltage corresponding to a five Gauss magnetic field. Magnetic field sensors, e.g., Hall effect sensors 402, continually or periodically sense magnetic field strength around the ferrous object and the magnetic proximity sensor. As the object is moved toward an operating MRI scanner, for example, the magnetic field output by the scanner increases in strength. Hall effect sensors 402 output a voltage corresponding to the sensed magnetic field strength. Comparators, e.g., comparators 408, compare the output voltage with the fixed voltage provided by potentiometer 404.
If the output voltage exceeds the fixed voltage (e.g., the external magnetic field exceeds the threshold magnetic field), decision 514, an alarm is triggered, in step 516. In an example of steps 514, 516, if the output voltage from Hall effect sensors 402 exceeds the fixed voltage from potentiometer 404, an alarm, e.g., alarm 406, is triggered and generates an alarm signal to alert personnel that the ferrous object has passed the five Gauss magnetic threshold, or safe point. If the external magnetic field weakens, e.g., the output voltage falls below the fixed voltage, decision 518, then the alarm stops, in step 520. In an example of steps 518, 520, the ferrous object is moved away from the MRI scanner such that the voltage output by sensor 402 drops below the fixed voltage provided by potentiometer 404. When the fixed voltage exceeds the voltage output by sensor 402, alarm 406 stops generating the alarm signal.
FIG. 9 is a flowchart depicting a method 550 of sensing a threshold magnetic field using a sensor with modified reed switches, e.g., as described with respect to FIGS. 5, 6A-7B. The sensor is attached to a ferrous object and turned on, in steps 452, 454. The sensor is exposed to a magnetic field, in step 456. In one example of steps 452-454, an MRI tech clips, sticks or otherwise fastens the sensor, e.g., sensor 420, FIG. 5, to a clipboard and brings the clipboard into an MRI suite. If the external magnetic field, for example generated by the MRI scanner, exceeds a threshold magnetic strength, decision 558, magnetic forces acting upon a ferromagnetic contact within a modified reed switch overcome stiffening properties of a monofilament or polymer supporting the ferromagnetic contact, and the contact is deflected by (bends toward or away from) the magnetic field, and closes a switch circuit, in step 560. In one example, external magnetic forces exert sufficient pull or push upon ferrous contact 434 to bend the contact and flex supporting sheath 442. Ferrous end or bead 436 contacts hemispheric contact 432 to close the circuit.
Closing of the circuit triggers an alarm, in step 562, which continues while the external magnetic field exceeds the threshold field strength, decision 464. Once the external field is less than the threshold strength, decision 464, the stiffening properties of the monofilament or polymer overcome magnetic attraction or repulsion of the ferrous contact, the ferrous contact returns to its original position, and the circuit opens, in step 566. The alarm stops, in step 568. In one example of steps 562-568, an audible, visible and/or tactile alarm 428 sounds when the circuit closes, in step 560. The above-mentioned MRI tech notes the alarm and moves the clipboard and the attached sensor 420 away from the MRI scanner. Once the sensor and clipboard are sufficiently far from the scanner that its magnetic forces fall below the sensor 420 threshold, pull exerted due to the stiffness of supporting sheath 442 overcomes magnetic forces acting upon ferrous contact 434, and returns contact 434 to its original, open position. Opening of the switch circuit stops alarm 428. Once the sensor, e.g., sensor 420 is turned off, alarm 428 will not operate, even though modified reed switches may continue to react to external magnetic fields.
Experimental Results
MRI machines serve as a major money making department of modern hospitals often grossing millions of dollars each year. In order to establish a basic understanding of the economics in the MRI department of a hospital, extensive interviews of various hospitals were conducted.
Hospitals in the United States and Europe (ranging in size from over a thousand in-patients to under one hundred) were interviewed to determine current MRI statistics such as average number of MRI patients, average number of MRI employees (doctors and staff), number of MRI units, standard safety precautions, including number of safety scanning checks, and staff/doctor time spent in screening patients prior to MRI procedures. Select results of these interviews are presented in Tables 1A and 1B, below.







TABLE 1A







Hospital Interviews: United States


Hospital Interviews: United States
















Number





Hospital/
Number

Working in
Number
Number of
Who is involved with the


Location
MRI units
Patients/Day
MRI
Doctors
Techs
screening process
















Penobscot Bay
1
  17.5
2
none
2 per shift;
questionnaire with tech


Rockport, ME



employed
travel with the
before entering room







MRI


Cooley
1
22
11
7
4
2 screenings; 1 questionnaire


Dickenson





over the phone and 1


Northhampton,





screening on site


MA


St. Vincent's
1
21
9
6 per shift
3 per shift
form with receptionist;


NY, NY





screening by tech


Holy Cross
1
15
7
4
3
questionnaire with 1 tech;


Silver Spring,





interview with another tech


MD


Archbold, M.C
1
20
7
4
not provided
questionnaire in waiting


Thomasville,





room; re-interview by tech


GA





before entering MRI


Florida
1

4
contract out
4
tech screens patient


Kissimmee, FL



to






radiologists


Memorial
2
27
8
staff
6
Checklist; interviewed by 1


Medical Center



radiologists

tech


Springfield, IL



(40)


Forest Park
1
not
4
staff
4
first screening with


St. Louis, MO

provided

radiologists

receptionist; review check








sheet with tech


Mercy
2
  27.5
16
10 
6
desk assistant screens,


Iowa City, IA





patients fills out form, then








tech interviews patient


Naval Medical
2
18



clerk checks questionnaire


San Diego, CA

per



and consults with tech before




scanner



entering MRI




per




day


Methodist
2
30
5
staff
10 total - 4
tech goes over questionnaire


Memphis,



radiologists
per shift
(10 mn)


Tennessee


MA General
6
65

staff
11 per week
two screenings once patient


Boston, MA



radiologists
day shift
arrives


Providence
2
60
16
6
9
tech goes over 1


Anchorage,





questionnaire per patient (5 min)


Alaska


Swedish
1
15
11
4 + staff
7
tech goes over questionnaire;


Medical Center



radiologists

different sheets for in


Seattle, WA





patient/ER patient/out patient








(10 min)


University of
4
35
16
Staff
13 
nurses screen then tech


Wisconsin



Radiologists

screens patients


Madison, WI



read the






images


St. John
1
25
5
Staff
5
techs screen in; in-patients


Detroit, MI



Radiologists

screened by nurses then






read the

again by techs.






images


Riverside
5
50
32
staff
12 specialized
MRI history screening -


Memorial



radiologists
MRI and 22
Tech goes over questionnaire


Columbus, OH




techs


Washoe Health
2
30
13
radiologist
10 
triple check system - 1


Reno, NV



on contract

questionnaire; 1 check sheet








with nurse; final check sheet








with tech


Methodist
1
80
10
staff
8 to 10
safety questionnaire must be


Houston, TX
(perm.




signed by two people who



mobile)




review - sometimes 2 techs








or 1 nurse 1 tech (10 mn)


Presbyterian
4
80-90
10
2 groups of
8 day/8 night/
tech; a whole department that


Hospital Dallas



staff
7 weekend
screens the patients; nurse


Dallas, TX



radiologists;

and tech screenings






(body MRI






and head






MRI)


Maui
1
15-25
5
Staff
4
Dr.; receptionist; last


Memorial




technologists
screening by techs (10 mn)


Medical Center


Wailuku, HI


DHMC
3, 1 is
55-65
7
staff
6 per shift
safety sheet; techs screen


Lebanon, NH
mobile
(with



before going into MRI (~10




mobile



mn)




unit)


Garrison
1
not
6
staff
1 travels with
traveling tech does final


Memorial

given

radiologists
MRI; hospital
screening


Garrison, ND



read images;
techs help if






1 main
needed.






radiologist






does MRI


Camp
1
21
5
staff
2 - come with
screened by 1 tech


Pendleton

(T-F)

radiologists
MRI unit


Camp

each

read the


Pendleton, CA

week

images


Scotland
1
 6
4
1 staff
3 come with
screened by 1 tech with a


County

(every

doctor
MRI
questionnaire


Memphis, MO

Tues.)


Jefferson
1
4-7
1 DR
1 radiologist
None from
tech and assistant - tech


County

(there
and 2
from
hospital - 2
finalizes interview before


Fairfield, IA

one
techs -
hospital
with MRI
patient is imaged.




day a
provided




week)
by





MRI





co.
















TABLE 1B







Hospital Interviews: Europe, Australia and New Zealand


Hospital Interviews: Europe, Australia and New Zealand

















Number






Hospital/
Number

Working in
Number
Number
Number
Who is involved with the


Location
MRI units
Patints/day
radiology
Doctors
Techs
Nurses
screening process?

















Queen Elizabeth II
2
30
3
1
2
0
Tech screen questionnaire -


Halifax, Nova






patients walk through metal


Scotia






detector, but the metal









detector is not used because









of its sensitivity. Metal









detector is about 9 years old.


Canadian
1
15
3
1
2
0
Techs screening


Diagnostic Center






questionnaire (standard) 10 mm


Halifax, Nova






procedure - refer to


Scotia






Frank Shellock's book on









MRI


Mater
1
12
4
1
3
0
Tech screening questionnaire -


Misericordiae

to




sometimes make patients


Dublin, Ireland

15




remove clothing to increase









resolution - have a metal









detector - don't use it - it is









not efficient - too sensitive


Balfast City
1
45/
5
Staff
4
0
Tech screening questionnaire


Belfast, N. Ireland

wk

radiologists


on phone and when they









come in


Western General
2 1-
30/
5
1
4
0
Tech screening questionnaire -


Edinburgh,
clinical
day




also use magnet to check


Scotland
1-





ferromagnetism



research


St. Michaels
2
40
7
staff
6
0
Tech screening questionnaire


Toronto, Canada
getting


radiologists


(10 mn)



a 3


St. Thomas
2
30
8
Staff
6
0
Tech screening questionnaire


London, U.K.



radiologists


(10 mn)


University
2
20
6
2
4
0
Tech screening


London, U.K.






Questionnaire - metal









detectors are useless - tried









one did not like it - too









sensitive


Middlesex
1
20
6
2
4
0
Tech screening questionnaire -


London, U.K.






magnet to check









ferromagnetism of objects


Derby Royal
1
30
5
10
4
0
Tech screening questionnaire -


Infirmary



Radiologist


magnet to check


Derby, U.K.



Staff


ferromagnetism of objects


Southern General
1
10
4
Staff
3
0
Tech screening questionnaire


Glasgow, Scotland



radiologists


(10 mn); problems with a









buffer accelerated into MRI









quenched magnet


DGH Royal
1
15/
3
1
2
0
Tech screening questionnaire


Shrusberry

visit




(10 mn)


Wales

wk


St. Vincent's
3
40-50
13
Staff
10
1
Tech screening questionnaire -


Melbourne,



radiologists


MRI technologist/nurse


Australia






(10-15mn); no metal









detectors (waste of time, too









sensitive). Shellock says the









detectors are inefficient.









Conferences in US and









Australia


Royal Perth
1
18-20
7
Staff
3
3
Tech screening questionnaire


Perth, Australia



radiologists


with nurse then again with









radiographer. Used metal









detector less than a month -









too sensitive, inefficient. Use









magnet to test









ferromagnetism - if the









inpatient may have metal but









doesn't know or if patient is









unable to be interviewed,









xrays are used to check









As shown in Tables 1A and 1B, a considerable amount of employee time is typically used in conducting multiple screening checks required by MRI facilities. In addition to these checks, MRI practitioners must take great care that no ferrous materials come close enough to the MRI scanner to be drawn into the bore of its magnet. Many MRI facilities use walk-through or other metal detectors at the entrance to an MRI suite. However, neither screenings nor metal detectors address the problems posed by metal (especially ferrous) objects that must be brought into proximity with a strong magnet, such as that used in an MRI scanner. The magnetic proximity sensor systems disclosed herein presents a solution to this problem. By attaching the magnetic proximity sensor system to ferrous objects that must be brought proximate the magnet, practitioners can be alerted when the ferrous object crosses a threshold “safe zone” of magnetic field strength.
Magnetic Proximity Sensor System Development and Test Results
The components considered and tested in developing one Magnetic Proximity Sensor system include:

    
    
        National Semiconductor LM139/LM239/LM3339/LM2901/LM3302 Low Power Low Offset Voltage Quad Comparators;
        National Semiconductor LM111/LM211/LM311 Voltage Comparators
        Texas Instruments TLC372, TLC372Q, TLC372Y LinCMOS Dual Differential Comparators
        Texas Instruments JG (R-GDIP-T8) Ceramic Dual-in-line
        Texas Instruments U (S-GDFP-F10) Ceramic Dual Flatpack
        Texas Instruments FK (S-CWCC-N) Leadless Ceramic Chip Carrier
        Texas Instruments P (R-PDIP-T8) Plastic Dual-in-line
        Texas Instruments D (R-PDSO-G) Plastic Small-outline Package
        Texas Instruments PS (R-PDSO-G8) Plastic Small-outline Package
        Texas Instruments PW (R-PDSO-G) Plastic Small-outline Package
        Copal Electronics Surface Mount Type Trimmers SM-4
        Axson Epopast 206
        Melexis MLX90215 Precision Programmable Linear Hall Effect Sensor
        Honeywell SS490 Series Hall Effect Sensors
        Honeywell 2SS52M Series Digital Magnetoresistive Sensors
        Honeywell HMC1023 3-Axis Magnetic Sensor
        Honeywell SR16/17 Hall Effect Vane Sensors
        Optek Hallogic® Hall Effect Sensors Types OHN3410U, OHS3140U, OH090U
        Panasonic Hall ICs DN6849/SE/S
        COTO Technology RI-80 SMD and RI-70 Series Dry Reed Switch
    
    


Sensors
Along with other analog sensors, both Reed switches and Hall effect sensors were investigated to determine their efficacy in detecting magnetic fields. Using an analog sensor allows for setting the sensor to detect a particular magnetic field Tested sensors include:







TABLE 2







Sensors tested for Magnetic Proximity Sensor








Company
Sensor





Melexis
Linear Hall Effect Sensor MLX90215 LC03



MLX90215LVA-LC03-ND


Honeywell
3-Axius Magnetic Sensor



Hall Effect Sensor SS495B


TT Electronics/OPTEX
Hall Effect Sensor 365-1003-ND


Technology (sold by
Hall Effect Sensor 365-1001-ND


DigiKey)
Hall Effect Sensor 296-10311-5-ND


Panasonic
Hall Effect Sensor DN6849S-ND


Coto Technology
Reed Switch R-170









Reed Switches

Testing of a prototype sensor and reviewing information about conventional reed switches indicated that reed switches may require modification for placement in a magnetic proximity sensor system. The metal contact plates inside the reed switches' glass casings can become magnetized by an MRI field, causing the alarm to sound even when removed from the magnetic field, or alternately, causing the alarm to stop sounding when returned to a magnetic field. The switches also proved fragile, non-resilient to bumps and tampering and ineffective for radial sensing.
The modified reed switch described above with respect to FIGS. 6A-7B may overcome these drawbacks. The single ferromagnetic contact described with respect to switches 422, 450, may reduce magnetization of the switch. The stiffening monofilament(s) or polymer(s) described above support and protect the ferromagnetic contact, and aid in returning the ferromagnetic contact to its original position upon appropriate reduction in an external magnetic field.
A Hall Effect Sensor generates an analog output voltage proportional to magnetic flux perpendicular to the magnetic field. This effect is created by passing an electrical current through the sensor while it is in the presence of a magnetic field.
A variety of Hall Effect sensors were tested, including those listed in Table 2. Single-direction Hall Effect sensors were first tested; and helped lay the circuit foundation for a prototype sensor system. Giant Magneto-Resistive Position Sensors were also tested, but exhibited higher sensitivity than needed for the Magnetic Proximity Sensor system (e.g., triggered and stopped the alarm at a Gauss level above the five Gauss default).
Magnetoresistive Position Sensors were likewise tested. When used in conjunction with an additional circuit amplifier, to maintain high voltage, these sensors may accurately detect the desired Gauss level; however, this adds to the overall size. Thus, magnetoresistive position sensors may be suitable in applications where the smallest possible device is not required. The 3-Axis Magnetic Sensor (HMC1023) was likewise tested; however, its higher cost may be prohibitive in some applications.
Bipolar Hall sensors (such as the Melexis' Linear Hall Effect Sensor MLX90215 LCO3) were found to provide accurate sensing in the x, y and z planes with three sensors, instead of six. This allowed for an overall smaller magnetic proximity sensor system that effectively detected and triggered the alarm at the five Gauss default level.
Alarm Buzzers
Decibel levels at various locations in an MRI department were measured to determine how loud the alarm buzzer must be to be heard over ambient noise. Tests were conducted in the MRI Department of Dartmouth-Hitchcock Medical Center, with the following results:







TABLE 3







Decibel Levels in MRI Facilities









Location/Activity
Sub-location In Room
Readings (dB)












MRI Room During Imaging
Near Door
78



Right of MRI Bench
80



Left of MRI Bench
79



End of MRI Bench
80








Average for MRI Room During Imaging
79.3









MRI Room, Ambient Noise
Near Door
58



Right of MRI Bench
58



Left of MRI Bench
60



End of MRI Bench
57








Average Ambient Noise for MRI Room
58.3









Hallway of MRI, Ambient Noise
Near Door
58



In Control Room
58



In Control Room
57



Outside Control Room
57








Average Ambient Noise for MRI Hallway
57.5









Patient Waiting Room,
Near Door
57


Ambient Noise
Right of MRI Bench
58



Left of MRI Bench
58



End of MRI Bench
57








Average Ambient Noise for Waiting Room
57.5









The Radio Shack 12VDC Piezo Mini Buzzer 273-074 provided an effective decibel output of 87.5 dB (louder than a typical household vacuum, which measures about 80 dB) and fit well into the size constraints of the Magnetic Proximity Sensor. Its range of 3.0-16V matched the voltage requirements of the Hall effect sensors. The test results provided in Table 3, indicate that the buzzer is significantly louder than the ambient noise of the MRI facility. At about 30 decibels higher than the ambient noises the buzzer is approximately to the power of 6 times the intensity of the ambient noise, loud enough to alert medical personnel to a problem if used in this facility.
As shown above, the MRI room during imaging has an average reading of 79.3 dB, which is much closer to the decibel level of the alarm buzzer. During the imaging process there should be no traffic into or out of the MRI room. It is unlikely that the magnetic proximity sensor would be used during the imaging process, as the door to the MRI suite would generally be closed and locked. However, in the unlikely event that the sensor is used during imaging, it is still almost 10 dB louder than the noise floor during imaging.
Potentiometers
Where Hall effect sensors are used, potentiometers may be required to create reference voltages sufficient to set off the alarm. Various potentiometers, including the Spectral 50K 43 P503 and the 10K Bourns 3262, were tested to see which created reference voltages sufficient to set off the tested buzzers at five Gauss.
The 10K Bourns 3262 Trimming Potentiometer, also known as a variable resistor, can be set by a user to a desired specific voltage. The potentiometer is also adjustable and can be changed when using different power supplies. Observation that the Hall sensors tested above had two outputs (one negative and one positive) and voltage measurements from these sensors indicated that two potentiometers would serve to provide fixed voltages. One potentiometer is for example set to provide a voltage corresponding to positive five Gauss and another set to provide a voltage corresponding to negative five Gauss.
Comparators
Comparators were used to check voltages from the sensors and compare the voltages to the set voltage of the variable resistors/potentiometers. The comparators for example compare the voltages to actuate the alarm buzzer(s). Single chip to quad comparators used in the development of this device include:







TABLE 4







Comparators tested for Magnetic Proximity Sensor









Company
Comparator Type/Size
Name/Part No.





National Semiconductor
single comparator chip,
LM311



size = 0.785 × 0.310 in.


National Semiconductor
quad (four) comparator chip
LM339



size = 0.785 × 0.310 in.









Simple conversions indicated that the magnetic proximity sensor usefully provide at least ten millivolts per Gauss. In testing the comparators, the Hall sensors were for example set at five Gauss and the comparators observed to detect fifty millivolts of change in the circuit voltage (which corresponds to 2.42V and 2.52V ((±5) Gauss).

The LM311 was first used in the prototype circuit; however, the LM339 was later adopted, for reasons of space conservation. The LM339 provides four comparators in a chip the same size as the one-comparator LM311. In addition to being designed to operate from a single power supply, the LM339 comparators have a low power drain.
Capacitors
Because Hall Effect sensors were set based on input and output voltages, capacitors were tested for their ability to minimize voltage variances in the circuit. Both μ10 farad and 0.1μ farad capacitors helped regulate voltage across circuit components, and were used in the final prototype.
Potting Material
The Rockwell hardness test was performed to assess the basic strength and resistance of silicon-type Epopast 206 and potting resin CR 300, in order to determine if they would function in a hospital environment. The Rockwell hardness test measures the bulk hardness of metallic and polymer materials, and correlates with strength and wear resistance. Rockwell Scale R, along with the 1⁄2 ball bit, was used to test the samples, with the following results:







TABLE 5







Results of Hardness Testing















Test 1
Test 2
Test 3
Test 4
Test 5
Test 6
Avg.


Material
(HRR)
(HRR)
(HRR)
(HRR)
(HRR)
(HRR)
(HRR)

















CR-300
12.7
14.3
13.2
12.0
12.2
12.8
12.87


(potting resin)












Epopast 206 (silicon)
too soft for these tests
0
0
0
0









Because the CR-300 Resin proved to be more resistant to wear and tear, it was chosen as the potting material for the Magnetic Proximity Sensor system prototype.

Prototype Components and Testing
Prototype Components
IC and surface mount prototype Magnetic Proximity Sensor systems were built using the following components:

    
    
        Melexis Linear Hall Effect Sensor MLX90215 LCO3
        Radio Shack 12VDC Piezo Mini Buzzer 273-074
        10K Bourns 3262 Trimming Potentiometer
        LM339 four-comparator chip
        10 μF capacitor
        0.1 μF capacitor
        potting resin CR 300
        Radio Shack Alkaline 6 Volt Battery (see “Batteries” subheading, below).
    
    


Batteries
Theoretical calculations were made to determine whether the prototype Magnetic Proximity Sensor system could be powered by EMF from an MRI machine, alone. Using Faraday's Law, we calculated the flux of a field that is the line integral of the magnitude of the field multiplied by the area of the coil moving through the field, according to Equation 1:




  
    
      
        
          
            d
            I
          
          
            d
            t
          
        
        =
        
          
            
              
                d
                B
              
              
                d
                t
              
            
            ⁢
            A
          
          +
          
            
              
                d
                A
              
              
                d
                t
              
            
            ⁢
            
              B
              .
            
          
        
      
    
    
      
        Eq
        .
        
          
        
        ⁢
        1
      
    
  




Because only one turn is being considered the equation becomes:





  
    
      
        
          
            d
            I
          
          
            d
            t
          
        
        =
        
          
            
              
                d
                B
              
              
                d
                x
              
            
            ·
            
              
                d
                x
              
              
                d
                t
              
            
          
          ⁢
          
            A
            .
          
        
      
    
    
      
        Eq
        .
        
          
        
        ⁢
        2
      
    
  




The change in magnitude of the field divided by the distance over which the field changes may be calculated by:





  
    
      
        
          
            
              d
              B
            
            
              d
              x
            
          
          -
          
            
              
                (
                
                  o
                  -
                  0.0003
                
                )
              
              ⁢
              T
            
            
              6.5
              ⁢
              
                
              
              ⁢
              m
            
          
        
        ,
      
    
    
      
        Eq
        .
        
          
        
        ⁢
        3
      
    
  




while velocity of the coil is found by:





  
    
      
        
          
            d
            x
          
          
            d
            t
          
        
        -
        
          
            
              1
              ⁢
              
                
              
              ⁢
              m
            
            
              2
              ⁢
              
                
              
              ⁢
              sec
            
          
          .
        
      
    
    
      
        Eq
        .
        
          
        
        ⁢
        4
      
    
  




Area of the coil is for example 0.000314 m2.

The EMF was calculated using the above equations and values. By substituting the dI/dt value into the following equations 5-7 relating EMF, resistance and current, power generated by the movement of the coil was determined.




  
    
      
        i
        =
        
          
            EMF
            
              
                R
                C
              
              +
              
                R
                L
              
            
          
          =
          
            
              7.25
              *
              
                10
                
                  -
                  8
                
              
              ⁢
              
                
              
              ⁢
              
                (
                
                  v
                  *
                  m
                
                )
              
            
            
              2
              ⁢
              
                
                  R
                  C
                
                ⁡
                
                  (
                  Ω
                  )
                
              
            
          
        
      
    
    
      
        Eq
        .
        
          
        
        ⁢
        5
      
    
  
  
    
      
        
          
            Power
            =
            
              EMF
              *
              I
            
          
          ;
        
        ⁢
        
          

        
        ⁢
        and
      
    
    
      
        Eq
        .
        
          
        
        ⁢
        6
      
    
  
  
    
      
        
          R
          c
        
        =
        
          
            
              (
              
                1.69
                ×
                
                  10
                  
                    -
                    8
                  
                
              
              )
            
            *
            
              
                (
                
                  2
                  ⁢
                  
                    π
                    ⁡
                    
                      (
                      r
                      )
                    
                  
                
                )
              
              
                π
                ⁢
                
                  
                
                ⁢
                
                  r
                  2
                
              
            
          
          =
          
            3.38
            ×
            
              10
              
                -
                6
              
            
            ⁢
            
              
            
            ⁢
            Ω
            ⁢
            
              /
            
            ⁢
            
              m
              .
            
          
        
      
    
    
      
        Eq
        .
        
          
        
        ⁢
        7
      
    
  




In order to obtain the greatest power RC and RL were set equal to each other. RC stands for the resistance of the cooper coil and RL is the resistance of the load, which allows the power to be removed from the coil. The resistance of copper wire is 1.69×10−8 Ω*m. Therefore the final equation for power used was:




  
    
      
        P
        =
        
          
            
              V
              2
            
            
              4
              ⁢
              
                R
                C
              
            
          
          =
          
            
              
                7.25
                *
                
                  10
                  
                    -
                    8
                  
                
                ⁢
                
                  
                
                ⁢
                
                  (
                  
                    v
                    *
                    m
                  
                  )
                
              
              
                1.352
                ×
                
                  10
                  
                    -
                    5
                  
                
                ⁢
                
                  
                
                ⁢
                Ω
                ⁢
                
                  /
                
                ⁢
                m
              
            
            .
          
        
      
    
    
      
        Eq
        .
        
          
        
        ⁢
        8
      
    
  




Substituting our values we obtain Power=0.00536 amps/s

The power required to run one prototype Magnetic Proximity Sensor system was calculated at about 0.02 V/s, using:

P=Volts*Current  Eq. 9.

This suggests that the prototype Magnetic Proximity Sensor system requires a power source in addition to the magnetic field of the MRI machine. The type of power source used for the Magnetic Proximity Sensor is important, for example because calibration of Hall effect sensors relies on the voltage through the circuit. Batteries ranging from various sized 3-volt coin cells to a small 6-volt alkaline battery were evaluated, including:








TABLE 6







Batteries tested for Magnetic Proximity Sensor











Company
Type
Name/Part No.







Radio Shack
Lithium 3 Volt Coin
CR2032CR2032





CR2450





CR1216



Radio Shack
6 Volt Alkaline
23-469










We found that the coin cell did not function at the correct voltage to support the Hall sensors, and thus focused on the alkaline battery. The 6-volt alkaline was in the voltage range required by the Melexis Hall effect sensors and small enough to fit into the mold for the device. Thus, the Radio Shack 6 Volt Alkaline 23-469 was incorporated into the prototype Magnetic Proximity Sensor system.
Prototype Testing
The prototype system was tested for sensing for radial sensing ability and for overall durability, shielding and accuracy.
Radial Sensing Tests
One of the key specifications of the MRI Gauss Detection Device is the ability to accurately sense a magnetic field in all directions, (x, y, z). Three-dimensional sensing was achieved by using three Hall effect sensors, one along each of the x, y and z axes. In order to ensure device accuracy, and to determine sensing capabilities and consistency of buzzer output, the prototype was tested every π/6 radians over a unit circle in the xy plane and the xz plane. The average distance from the center of the magnet with a field strength of five Gauss was 10.5 centimeters. The device was moved over the circle with a radius of 10.5 cm. At every π/6, the Gauss reading and the decibel output of the device was recorded. Table 7, below, illustrates the angles at which radial sensing was tested.







TABLE 7




















As shown in Tables 8 and 9, below, the radial sensing test results indicate that the prototype system accurately senses at every π/6. The deviations in buzzer output along the circle in the xy and xz plane were 1.28 dB and 1.97 dB, respectively. This deviation is negligible, and the tests show that buzzer output was constant for the ranges tested.







TABLE 8







Radial Sensing in xy Plane












Distance from
Field
Decibel
Deviation in


Degree measure
Sensor
Strength
Output
Decibel


xy plane
(cm)
(Gauss)
(dB)
Output


Degree
Distance
Field
Decibel
Deviation in


measure
from
Strength
Output
Decibel


xy plane
Sensor (cm)
(Gauss)
dB
Output














0
10.5
5.0
88
.4


π/6
10.5
5.0
88
.4


π/3
10.5
4.9
87
.6


π/2
10.5
5.1
88
.4


2π/3
10.5
5.2
86
1.6


5π/6
10.5
4.9
86
1.6


π
10.5
5.1
88
.4


7π/6
10.5
4.9
86
1.6


4π/3
10.5
5.0
88
.4


3π/2
10.5
5.2
84
3.6


5π/3
10.5
4.9
88
.4


11π/6
10.5
5.0
88
.4


2π
10.5
5.0
88
.4


Averages
10.5
5.0
87.6
1.28
















TABLE 9







Radial Sensing in xz Plane











Degree
Distance from

Decibel
Deviation in


measure
Sensor
Field Strength
Output
Decibel


xz plane
(cm)
(Gauss)
(dB)
Output














0
10.5
4.9
88
.8


π/6
10.5
5.2
86
1.2


π/3
10.5
5.2
88
.8


π/2
10.5
5.1
90
2.8


2π/3
10.5
5.0
91
3.8


5π/6
10.5
4.8
88
.8


π
10.5
4.9
84
3.2


7π/6
10.5
4.9
85
2.2


4π/3
10.5
5.0
89
1.8


3π/2
10.5
5.1
88
.8


5π/3
10.5
5.1
89
1.8


11π/6
10.5
5.1
88
.8


2π
10.5
4.9
86
1.2


Averages
10.5
5.0
87.2
1.97









Material Testing

Results of testing for accuracy, shielding and durability are given in Tables 10-12, below.







TABLE 10







Accuracy Test Results









Trial
five Gauss (Y/N*)
4 Gauss (Y/N*)












1
Yes
No


2
Yes
No


3
Yes
No


4
Yes
No


5
Yes
No


6
Yes
No


7
Yes
No


8
Yes
No


9
Yes
No


10
Yes
No
















TABLE 11







Shielding Test Results










Material
five Gauss (Y/N*)







Aluminum (1 mm)
Yes



Plastic (2 mm)
Yes



Skin (hand)
Yes



Clothing
Yes



Plexiglas (0.5 cm)
Yes



Wood (1.8 cm)
Yes



Rubber (7 mm)
Yes

















TABLE 12







Durability Test Results












Dropping (6






inches)
Worked (Y/N*)
Banged
Worked (Y/N*)
















1
Yes
1
Yes



2
Yes
2
Yes



3
Yes
3
Yes



4
Yes
4
Yes



5
Yes
5
Yes



6
Yes
6
Yes



7
Yes
7
Yes



8
Yes
8
Yes



9
Yes
9
Yes



10
Yes
10
Yes







*Yes means the device still worked as the baseline.






Since certain changes may be made in the above methods and systems without departing from the scope hereof, it is intended that all matter contained in the above description or shown in the accompanying drawing be interpreted as illustrative and not in a limiting sense. It is also to be understood that the following claims are to cover certain generic and specific features described herein.

## Claims

1. A magnetic proximity sensor system, comprising:
at least one modified reed switch having:
a switch housing;
a conductive hemispheric contact secured within the switch housing;
a magnetic contact having a first end anchored with the switch housing and a second end centered with the hemispheric contact; and
a stiffening filament for supporting the magnetic contact; the stiffening filament being sufficiently flexible to bend when an external magnetic force of a preselected strength deflects the magnetic contact;

wherein the magnetic contact is deflected into connection with the hemispheric contact, to close a switch circuit; and
wherein an external magnetic force of sufficient strength to overcome the supportive stiffening filament deflects the magnetic contact and flexes the stiffening filament, the second end contacting the hemispheric contact to close a switch circuit.

2. The sensor system of claim 1, further comprising:
an alarm in communication with the at least one reed switch, for generating an alarm signal when the switch circuit closes;
a housing for protecting the at least one reed switch and the alarm; and
an electrical contact for connecting to a battery or external power source, for powering the alarm.

3. The sensor system of claim 2, wherein the conductive hemispheric contact is non-magnetic.

4. A modified reed switch, comprising:
a housing;
a conductive hemispheric contact secured within the housing;
a magnetic contact having a first end anchored with the housing and a second end centered with the hemispheric contact; and
a stiffening filament for supporting the magnetic contact, the stiffening filament chosen to withstand flexing due to external magnetic forces acting upon the magnetic contact, up to a selected threshold magnetic field strength;
wherein under magnetic fields above the threshold strength, deflection of the magnetic contact bends the stiffening filament and the second end of the magnetic contact contacts the hemispheric contact to close a switch circuit.

5. The sensor system of claim 4, the conductive hemispheric contact comprising one or more supports for stabilizing the hemispheric contact within the switch housing.

6. The sensor system of claim 4, the conductive hemispheric contact comprising a wire extending through the switch housing.

7. The sensor system of claim 4, the magnetic contact selected from the group of:
a ferromagnetic reed; and
a wire with a ferrous bead at the second end.

8. The sensor system of claim 4, the magnetic contact comprising a wire with a ferrous bead at the second end, the stiffening filament comprising a first filament connected with the bead and with an end of the switch housing; further comprising a second stiffening filament connected with an opposite end of the switch housing and with the bead, opposite the first filament.

9. The sensor system of claim 4, the stiffening filament comprising a sheath for supporting the magnetic contact, the second end of the magnetic contact extending from the sheath.

10. The sensor system of claim 4, the magnetic contact comprising a wire with a ferrous bead at the second end; further comprising a conductive wire connected with the bead at one end, a second end of the conductive wire extending through the switch housing.

11. The sensor system of claim 10, the second end of the conductive wire connecting with an electrical contact external to the switch housing.

12. The sensor system of claim 4, the stiffening filament comprising a polymer.

13. The sensor system of claim 4, wherein the stiffening filament is manufactured to flex when a magnetic field of a selected strength acts upon the magnetic contact.

14. The sensor system of claim 2, the alarm selected from the group consisting of an audible alarm, a visual alarm and a tactile alarm.

15. The sensor system of claim 2, the alarm comprising an audible alarm; further comprising a speaker for playing the audible alarm.

16. The sensor system of claim 1, the stiffening filament chosen to withstand flexing due to external magnetic forces acting upon the magnetic contact, up to a selected threshold magnetic field strength.

17. The sensor system of claim 2, the housing comprising means for securing the sensor to a person or to a movable metal object.

18. The sensor system of claim 1, the conductive hemispheric contact comprising one or more supports for stabilizing the hemispheric contact within the switch housing.

19. The sensor system of claim 1, the conductive hemispheric contact comprising a wire extending through the switch housing.

20. The sensor system of claim 1, the magnetic contact selected from the group of:
a ferromagnetic reed; and
a wire with a ferrous bead at the second end.

21. The sensor system of claim 1, the magnetic contact comprising a wire with a ferrous bead at the second end, the stiffening filament comprising a first filament connected with the bead and with an end of the switch housing; further comprising a second stiffening filament connected with an opposite end of the switch housing and with the bead, opposite the first filament.

22. The sensor system of claim 1, the stiffening filament comprising a sheath for supporting the magnetic contact, the second end of the magnetic contact extending from the sheath.

23. The sensor system of claim 1, the magnetic contact comprising a wire with a ferrous bead at the second end; further comprising a conductive wire connected with the bead at one end, a second end of the conductive wire extending through the switch housing.

24. The sensor system of claim 23, the second end of the conductive wire connecting with an electrical contact external to the switch housing.

25. The sensor system of claim 1, the stiffening filament comprising a polymer.